JPH0365686B2 - - Google Patents

Info

Publication number
JPH0365686B2
JPH0365686B2 JP58056350A JP5635083A JPH0365686B2 JP H0365686 B2 JPH0365686 B2 JP H0365686B2 JP 58056350 A JP58056350 A JP 58056350A JP 5635083 A JP5635083 A JP 5635083A JP H0365686 B2 JPH0365686 B2 JP H0365686B2
Authority
JP
Japan
Prior art keywords
power supply
voltage
circuit
transistor
collector
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired - Lifetime
Application number
JP58056350A
Other languages
Japanese (ja)
Other versions
JPS59182623A (en
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed filed Critical
Priority to JP58056350A priority Critical patent/JPS59182623A/en
Publication of JPS59182623A publication Critical patent/JPS59182623A/en
Publication of JPH0365686B2 publication Critical patent/JPH0365686B2/ja
Granted legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H03ELECTRONIC CIRCUITRY
    • H03KPULSE TECHNIQUE
    • H03K5/00Manipulating of pulses not covered by one of the other main groups of this subclass
    • H03K5/153Arrangements in which a pulse is delivered at the instant when a predetermined characteristic of an input signal is present or at a fixed time interval after this instant
    • H03K5/1536Zero-crossing detectors
    • HELECTRICITY
    • H03ELECTRONIC CIRCUITRY
    • H03KPULSE TECHNIQUE
    • H03K17/00Electronic switching or gating, i.e. not by contact-making and –breaking
    • H03K17/13Modifications for switching at zero crossing

Landscapes

  • Physics & Mathematics (AREA)
  • Nonlinear Science (AREA)
  • Manipulation Of Pulses (AREA)
  • Electronic Switches (AREA)

Description

【発明の詳細な説明】 本発明は、交流電流の回路を開閉する場合にお
いて、その交流電流の零電位附近で電路を開閉す
ることによりスパークの防止と、スイツチ・オン
時における突入電流の軽減を計るための交流零電
位開閉回路に関するものである。
DETAILED DESCRIPTION OF THE INVENTION When opening and closing an alternating current circuit, the present invention prevents sparks and reduces inrush current when a switch is turned on by opening and closing the electrical circuit near the zero potential of the alternating current. This relates to an AC zero potential switching circuit for measurement.

即ち、本発明は、双方向導通サイリスタの主電
路を介して負荷に接続された交流電源からの電圧
を抵抗を通じてトランジスタのベース電極とエミ
ツタ電極との間に印加し、コレクタ電流を交流電
源と同じ周波数の矩形波として、コレクタまたは
エミツタからトランスまたはコンデンサ結合回路
により双方向導通サイリスタのゲート電極へ制御
用電流を供給すると共に、トランジスタのコレク
タ電圧は、交流電源からスイツチを経て、整流用
ダイオードと抵抗により交流電源周波数の数分の
1の時定数を持つ平滑回路で直流化し、スイツ
チ・オンの時から直流電圧が上昇するようにした
ことを特徴とする交流零電位開閉回路を要旨とす
るものである。
That is, the present invention applies a voltage from an AC power supply connected to a load through a main circuit of a bidirectional conduction thyristor through a resistor between a base electrode and an emitter electrode of a transistor, so that the collector current is the same as that of the AC power supply. A control current is supplied as a square wave of the frequency from the collector or emitter to the gate electrode of the bidirectional conduction thyristor by a transformer or capacitor coupling circuit, and the collector voltage of the transistor is supplied from the AC power supply via a switch to a rectifier diode and a resistor. The gist of this is an AC zero-potential switching circuit, which is characterized in that it converts to DC using a smoothing circuit with a time constant that is a fraction of the AC power frequency, and the DC voltage increases from the time the switch is turned on. be.

第1図において、交流電源ACの電圧を端子U
から抵抗R3を経てトランジスタTのベース電極
に高電圧として印加する。そのため、トランジス
タTの出力は常に飽和状態となつて第5図ロに示
すような矩形波出力が得られる。
In Figure 1, the voltage of AC power supply AC is connected to terminal U.
A high voltage is applied to the base electrode of the transistor T through the resistor R3 . Therefore, the output of the transistor T is always in a saturated state, and a rectangular wave output as shown in FIG. 5B is obtained.

このトランジスタTにおける矩形波出力をトラ
ンスHを介して、その2次側の電圧波形を第5図
ハのようにし第5図イの交流電源ACにおける交
流電圧の零点と合致するようにする。
The rectangular wave output from the transistor T is passed through the transformer H so that the voltage waveform on the secondary side thereof is made as shown in FIG.

この電圧を第1図の双方向導通サイリスタKの
ゲート電極に印加することによつて、交流電源
ACにおける交流電圧の立上り点からトリガーさ
れ導通状態となる。
By applying this voltage to the gate electrode of the bidirectional conduction thyristor K shown in FIG.
It becomes conductive when triggered from the rising point of AC voltage.

また、第1図において端子U側のスイツチSを
閉じると、ダイオードDから抵抗R1を経てコン
デンサCに充電され、その充電曲線は第5図ニの
ように数ヘルツ後に定常電圧となる。この時定数
は、抵抗R1,R2およびコンデンサCの値によつ
て定まる。
When the switch S on the terminal U side in FIG. 1 is closed, the capacitor C is charged from the diode D through the resistor R1 , and the charging curve becomes a steady voltage after several hertz as shown in FIG. 5D. This time constant is determined by the values of resistors R 1 , R 2 and capacitor C.

第1図におけるトランジスタTのコレクタ電圧
は、第5図ニのような電圧となるため、その出力
は第5図ロのように最初は低く除々に波高が増し
てゆくことになる。そのため微分した出力も第5
図ハに示すように除々に増加してゆき、双方向導
通サイリスタKのトリガーレベルに達したモード
のゲート電圧のときだけ双方向導通サイリスタK
は導通となるため、その電流は第5図ホのよう
に、最初の2ヘルツは半波電流であり、第3ヘル
ツから全波電流が流れることとなる。ただし、時
定数を少なくすればスイツチ・オンと同時に双方
向導通サイリスタKは働くことになる。
Since the collector voltage of the transistor T in FIG. 1 becomes a voltage as shown in FIG. 5 (d), its output is initially low and the wave height gradually increases as shown in FIG. 5 (b). Therefore, the differentiated output is also the fifth
As shown in Figure C, the gate voltage of the bidirectional conduction thyristor K increases gradually, and only when the mode gate voltage reaches the trigger level of the bidirectional conduction thyristor K.
becomes conductive, so the current is a half-wave current for the first two hertz, and a full-wave current flows from the third hertz, as shown in FIG. 5(e). However, if the time constant is reduced, the bidirectional conducting thyristor K will work at the same time as the switch is turned on.

第2図に示すものは、第1図と基本的に同じで
あるが、トランジスタTの出力をエミツタ・フオ
ローで得ているものであるから、小電流で作動す
る双方向導通サイリスタKを使用するのに好適で
ある。図中のコンデンサC2は矩形波を微分波形
とするためのものである。
The one shown in Figure 2 is basically the same as Figure 1, but since the output of the transistor T is obtained by emitter follow, a bidirectional conduction thyristor K that operates with a small current is used. It is suitable for Capacitor C2 in the figure is for converting the rectangular wave into a differential waveform.

このように、第1図、第2図に示す回路とも、
スイツチSを閉じると交流の立上り点から導通状
態となり、スイツチSを開くと交流電流の立下り
点で不導通状態となるため、スイツチSの開閉時
に火花放電を皆無とすることができる。
In this way, both the circuits shown in FIGS. 1 and 2,
When the switch S is closed, it becomes conductive from the rising point of the alternating current, and when the switch S is opened, it becomes non-conductive at the falling point of the alternating current, so that spark discharge can be completely eliminated when the switch S is opened and closed.

第1図、第2図における回路定数の1例を示せ
ば、次の通りである。
An example of circuit constants in FIGS. 1 and 2 is as follows.

交流電源ACは100ボルトまたは200ボルトであ
り、抵抗R1は5キロオームまたは10キロオーム、
抵抗R2は50キロオーム、抵抗R3は100キロオーム
または200キロオーム、そしてコンデンサCは10
〜100マイクロフアラツドである。
The alternating current power supply AC is 100 volts or 200 volts, and the resistor R 1 is 5 kilo ohms or 10 kilo ohms,
Resistor R 2 is 50 kilo ohms, resistor R 3 is 100 kilo ohms or 200 kilo ohms, and capacitor C is 10
~100 microfarads.

また、図中のZは負荷抵抗であつて、例えば電
球、電熱器、モーターなどの各種電気器具であ
り、双方向導通サイリスタKの主電路を介して交
流電源ACに接続されている。
Further, Z in the figure is a load resistance, which is, for example, various electric appliances such as a light bulb, an electric heater, and a motor, and is connected to an alternating current power supply AC through a main circuit of a bidirectional conduction thyristor K.

さらにまた、第1図、第2図においてコンデン
サCと抵抗R1,R2の値によつて、スイツチSを
閉じた瞬間に回路を導通させ負荷抵抗Zとなる各
種の電気器具をスタートさせることも可能であ
る。
Furthermore, depending on the values of the capacitor C and the resistors R 1 and R 2 in FIGS. 1 and 2, the circuit is made conductive at the moment the switch S is closed, and various electrical appliances serving as the load resistance Z are started. is also possible.

第3図に示すものは、トランジスタTのエミツ
タ電極にトランスHを結合したエミツタ・フオロ
アー方式の回路であり、第4図に示すものは、ト
ランジスタTのコレクタに抵抗R5とコンデンサ
C3とを結合した回路であり、必要によつて適宜
な回路を採用し得る。
The circuit shown in Figure 3 is an emitter-follower type circuit in which a transformer H is coupled to the emitter electrode of the transistor T, and the circuit shown in Figure 4 is a circuit with a resistor R5 and a capacitor connected to the collector of the transistor T.
This is a circuit that combines C3 , and an appropriate circuit can be adopted as necessary.

【図面の簡単な説明】[Brief explanation of drawings]

図は本発明の実施例を示し、第1図は時定数を
持つた整流回路の電圧でトランジスタと双方向導
通サイリスタとを駆動する方式の回路図、第2図
はトランジスタのエミツタ・フオロアー方式の回
路図、第3図はトランジスタのエミツタ・フオロ
アーにトランスを結合した回路図、第4図はトラ
ンジスタのコレクタに抵抗とコンデンサを結合し
た回路図、第5図は電圧、電流の波形図である。 図中の符号を説明すれば、次の通りである。
ACは交流電源、Tはトランジスタ、Rは低坑、
Cはコンデンサ、Hはトランス、Dはダイオー
ド、Kは双方向導通サイリスタ、Sはスイツチ、
Zは負荷抵抗。
The figures show embodiments of the present invention. Fig. 1 is a circuit diagram of a system in which a transistor and a bidirectional conduction thyristor are driven by the voltage of a rectifier circuit having a time constant, and Fig. 2 is a circuit diagram of a system in which a transistor and a bidirectional conducting thyristor are driven. FIG. 3 is a circuit diagram in which a transformer is coupled to the emitter follower of a transistor, FIG. 4 is a circuit diagram in which a resistor and a capacitor are coupled to the collector of a transistor, and FIG. 5 is a voltage and current waveform diagram. The symbols in the figure are explained as follows.
AC is alternating current power supply, T is transistor, R is low voltage,
C is a capacitor, H is a transformer, D is a diode, K is a bidirectional conduction thyristor, S is a switch,
Z is load resistance.

Claims (1)

【特許請求の範囲】[Claims] 1 双方向導通サイリスタの主電路を介して負荷
に接続された交流電源からの電圧を抵抗を通じて
トランジスタのベース電極とエミツタ電極との間
に印加し、コレクタ電流を交流電源と同じ周波数
の矩形波として、コレクタまてはエミツタからト
ランスまたはコンデンサ結合回路により双方向導
通サイリスタのゲート電極へ制御用電流を供給す
ると共に、トランジスタのコレクタ電圧は、交流
電源からスイツチを経て、整流用ダイオードと抵
抗により交流電源周波数の数分の1の時定数を持
つ平滑回路で直流化し、スイツチ・オンの時から
直流電圧が上昇するようにしたことを特徴とする
交流零電位開閉回路。
1 The voltage from the AC power supply connected to the load through the main circuit of the bidirectional conduction thyristor is applied between the base electrode and emitter electrode of the transistor through the resistor, and the collector current is converted into a rectangular wave with the same frequency as the AC power supply. , a control current is supplied from the collector or emitter to the gate electrode of the bidirectional conduction thyristor by a transformer or capacitor coupling circuit, and the collector voltage of the transistor is transferred from the AC power supply via a switch to the AC power supply by a rectifier diode and a resistor. An alternating current zero potential switching circuit characterized by converting to direct current using a smoothing circuit with a time constant that is a fraction of the frequency so that the direct current voltage increases from the time the switch is turned on.
JP58056350A 1983-03-31 1983-03-31 Ac zero potential switching circuit Granted JPS59182623A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP58056350A JPS59182623A (en) 1983-03-31 1983-03-31 Ac zero potential switching circuit

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP58056350A JPS59182623A (en) 1983-03-31 1983-03-31 Ac zero potential switching circuit

Publications (2)

Publication Number Publication Date
JPS59182623A JPS59182623A (en) 1984-10-17
JPH0365686B2 true JPH0365686B2 (en) 1991-10-14

Family

ID=13024777

Family Applications (1)

Application Number Title Priority Date Filing Date
JP58056350A Granted JPS59182623A (en) 1983-03-31 1983-03-31 Ac zero potential switching circuit

Country Status (1)

Country Link
JP (1) JPS59182623A (en)

Also Published As

Publication number Publication date
JPS59182623A (en) 1984-10-17

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